Abstract:A numerical methodology is proposed for the calculation of transient electromagnetic interference induced by overhead high-voltage power lines in metallic structures buried in soil—pipelines for oil or gas transportation. A series of 2D finite element simulations was employed to sample the harmonic response of a given geometry section. The numerical inverse Laplace transform of the results allowed obtaining the time domain evolution of the induced voltages and currents in the buried conductors, for any given c… Show more
“…The right-hand-side of (56) represents the computation that the function f needs to perform. Since the JIT Matlab compiler is not always able to handle loops with complex expressions efficiently [50], [51], the implementation of the function f was extensively vectorized, aiming at reducing computational time. A drawback of using the implicit approach is that the output of the ode23tb function is the state vector at every required time instant.…”
In recent years, the use of HVDC cables has grown exponentially. One of the main challenges that remains concerns the space charge accumulation inside the insulating materials. A better understanding of the mechanisms governing this phenomenon is essential to improve the performance of HVDC systems. Numerical simulations are often employed to achieve this goal. For this reason, it is important to perform them in an efficient way. In this work, we test several numerical techniques, aiming to assess which one is the best to use for fast and reliable simulations. We consider a well-known bipolar dynamic model from the literature for our simulations. The model considers a single level of deep traps and is implemented in a one-dimensional Cartesian coordinate system, considering a thin specimen of polymeric material. We compare three different time discretization methods: a fully explicit, a semi-implicit, and a fully implicit approaches. For the advective flux discretization, we compare the first-order upwind scheme (FOU) with a second-order upwind scheme coupled with the Koren flux limiter (SOU/KL). Regarding the computation of the polarization current, we introduce a simple approach using Sato's equation and compare it with the well-established approach based on the total current density.INDEX TERMS Bipolar charge transport, Koren flux limiter, polymeric dielectrics, drift diffusion, polarization current, numerical simulation, efficient computation.
“…The right-hand-side of (56) represents the computation that the function f needs to perform. Since the JIT Matlab compiler is not always able to handle loops with complex expressions efficiently [50], [51], the implementation of the function f was extensively vectorized, aiming at reducing computational time. A drawback of using the implicit approach is that the output of the ode23tb function is the state vector at every required time instant.…”
In recent years, the use of HVDC cables has grown exponentially. One of the main challenges that remains concerns the space charge accumulation inside the insulating materials. A better understanding of the mechanisms governing this phenomenon is essential to improve the performance of HVDC systems. Numerical simulations are often employed to achieve this goal. For this reason, it is important to perform them in an efficient way. In this work, we test several numerical techniques, aiming to assess which one is the best to use for fast and reliable simulations. We consider a well-known bipolar dynamic model from the literature for our simulations. The model considers a single level of deep traps and is implemented in a one-dimensional Cartesian coordinate system, considering a thin specimen of polymeric material. We compare three different time discretization methods: a fully explicit, a semi-implicit, and a fully implicit approaches. For the advective flux discretization, we compare the first-order upwind scheme (FOU) with a second-order upwind scheme coupled with the Koren flux limiter (SOU/KL). Regarding the computation of the polarization current, we introduce a simple approach using Sato's equation and compare it with the well-established approach based on the total current density.INDEX TERMS Bipolar charge transport, Koren flux limiter, polymeric dielectrics, drift diffusion, polarization current, numerical simulation, efficient computation.
“…This allows one to compute the time-evolution of one of the quantities yielded by the FEM solver, using solutions computed in the complex domain. This formulation is closely related to the quasi-stationary formulation, substituting the purely imaginary jω with the complex variable s. Details of this approach can be found in [31] and are briefly summarized below.…”
“…The main novelties of this work are the vectorized implementation of two solvers for quasi-magnetostatic transient problems, the subsequent comparison and numerical validation of the two approaches, and the benchmarking of three inverse-Laplace routines included in FLARE. The approach based on the inverse-Laplace technique was introduced by the authors in [31]. A similar technique was also recently employed to study quasi-electrostatic problems in [32] and has been applied to other problems in the past, such as unsteady heat flow calculations [33].…”
Section: Introduction Concerns Over Metallic Pipelines Integritymentioning
confidence: 99%
“…A similar technique was also recently employed to study quasi-electrostatic problems in [32] and has been applied to other problems in the past, such as unsteady heat flow calculations [33]. The work in [31] was focused on the theoretical development of the method, and the developed code was based on a serial Fortran 90 inversion routine by D'Amore et al [34]. In this work, we integrate the approach into the FLARE framework, providing a fully parallelized (shared memory) and more flexible MATLAB ® implementation of the routines.…”
Section: Introduction Concerns Over Metallic Pipelines Integritymentioning
confidence: 99%
“…We also add two additional (parallel) inversion routines, based on the work of Abate et al [35]; as will be shown in a dedicated section of this work, these techniques are somewhat complementary to that by D'Amore and colleagues, from an accuracy and computational efficiency perspective. With respect to the work in [31], here we want to provide a numerical validation of the inverse-Laplace solution for a transient problem. To do that, we also implement a quasi-magnetostatic solver based on a time-marching procedure, which can operate with either fixed or variable time step lengths; we directly validate the time-marching solution against the solution yielded by the AC/DC module of COMSOL Multiphysics ® on the same problem.…”
Section: Introduction Concerns Over Metallic Pipelines Integritymentioning
The functionality of buried metallic pipelines can be compromised by the electrical lines that share the same right-of-way. Given the considerable size of shared corridors, computer simulation is an important tool for performing risk assessment and mitigation design. In this work, we introduce an open-source computational framework for the analysis of electromagnetic interference on large earth-return structures. The developed framework is based on FLARE—an efficient finite element solver developed by the authors in MATLAB®. FLARE includes solvers for problems involving static electric and magnetic fields, and DC and time-harmonic AC currents. Quasi-magnetostatic transient problems can be studied through time-marching or—for linear problems—with an efficient inverse-Laplace approach. In this work, we succinctly describe the optimization of time-critical operations in FLARE, as well as the implementation of a transient solver with automatic time-stepping. We validate the numerical results obtained with FLARE via a comparison with the commercial software COMSOL Multiphysics®. We then use the validated time-marching analysis results to test the accuracy and efficiency of three numerical inverse-Laplace algorithms. The test problem considered is the assessment of the inductive coupling between a 500 kV transmission line and a metallic pipeline buried in the soil.
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